Method of amplifying work output to be greater than work input using a fully mechanical system
Abstract
A mechanical energy amplification system and method, where the system includes a frame that supports a cylindrical rotary reactor magnet assembly, an oscillating reactor magnet assembly, and an input impulse magnet assembly. The input impulse magnet assembly rotates an axial shaft connected to both the rotary reactor magnet assembly and a flywheel, and the oscillating reactor magnet assembly when pivoted back and forth, and generates a greater output energy than an energy input at the input impulse magnet assembly by increasing the pivoting of and torque of an output pivot shaft by the rotation of the shafts of the rotary reactor magnet assembly and the oscillating reactor magnet assembly.
Claims
exact text as granted — not AI-modifiedWhat is claimed is:
1. A method of amplifying input energy to produce greater output energy, the method comprising:
rotating a shaft axially extending from a cylindrical rotary reactor magnet assembly and a shaft axially extending from a cylindrical oscillating reactor magnet assembly simultaneously by pivoting back and forth a cylindrical input impulse magnet assembly disposed between the cylindrical rotary reactor magnet assembly and the cylindrical oscillating reactor magnet assembly;
rotating a flywheel with the rotation of the shaft axially extending from the cylindrical rotary reactor magnet assembly;
pivoting a flywheel crank drive link back and forth with the rotation of the shaft axially extending from the cylindrical rotary reactor magnet assembly and the rotation of the flywheel;
pivoting an oscillating reactor magnet power rod back and forth with the rotation of the shaft axially extending from the oscillating reactor magnet assembly; and
pivoting an output main motor shaft back and forth with the pivoting of the flywheel crank drive link and the pivoting of the oscillating reactor magnet power rod.
2. The method according to claim 1 , wherein the cylindrical input impulse magnet assembly is pivoted back and forth within a 30 degree range of rotation.
3. The method according to claim 1 , wherein the flywheel crank drive link is pivoted back and forth by a flywheel crank fixedly connected at one end thereof to the shaft axially extending from a cylindrical rotary reactor magnet assembly and flywheel and connected to a rotatable bearing connected to one end of the flywheel crank drive link.
4. The method according to claim 1 , wherein the output main motor shaft is pivoted about an output pivot shaft trunnion disposed at a center of the output main motor shaft.
5. The method according to claim 4 , wherein the output main motor shaft is pivoted at one end thereof by the flywheel crank drive link and at an opposite end thereof by the oscillating reactor magnet power rod.
6. The method according to claim 4 , wherein the input impulse magnet assembly, the rotary reactor magnet assembly, the oscillating reactor magnet assembly and the output pivot shaft trunnion rotate about bearings.
7. The method according to claim 1 , wherein the cyclic load of the output of the output pivot shaft increases disproportionately to the pivoting force applied to the cylindrical input impulse magnet assembly.
8. The method according to claim 1 , wherein the kinetic energy stored in the flywheel increases disproportionately to the pivoting force applied to the cylindrical input impulse magnet assembly.
9. A method of generating an increasing output energy from a mechanical system by applying a pre-set input energy to the mechanical system, the method comprising:
applying a magnetic force to a first magnetic cylinder and a second magnetic cylinder simultaneously to rotate the first and second magnetic cylinders;
applying a rotational force to a flywheel with a rotational force of the first magnetic cylinder;
applying an oscillating force to a flywheel crank drive link with the rotational force of the flywheel;
applying a pivoting force to a first end of an output main motor shaft with the oscillating force of the flywheel crank drive link;
applying an oscillating force to an oscillating power rod with the rotational force of the second magnetic cylinder; and
applying a pivoting force to a second end of the output main motor shaft with the oscillating force of the oscillating power rod.
10. The method according to claim 9 , wherein the applying a magnetic force to a first magnetic cylinder and a second magnetic cylinder simultaneously to rotate the first and second magnetic cylinders is performed by pivoting an impulse magnet assembly back and forth within a range of approximately 60 degrees.
11. The method according to claim 10 , wherein the total torque output equals the sum of the torque from the kinetic energy of the flywheel and torque generated by the first magnetic cylinder and a second magnetic cylinder.Join the waitlist — get patent alerts
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